(a) Equation (17.12) gives the stress required to keep the length of a rod constant as its temperature changes. Show that if the length is permitted to change by an amount Δ L when its temperature changes by Δ T , the stress is equal to F A = Y ( Δ L L 0 − α Δ T ) where F is the tension on the rod, L 0 is the original length of the rod, A its cross-sectional area, α its coefficient of linear expansion, and Y its Young’s modulus. (b) A heavy brass bar has projections at its ends ( Fig. P17.79 ). Two fine steel wires, fastened between the projections, are just taut (zero tension) when the whole system is at 20°C. What is the tensile stress in the steel wires when the temperature of the system is raised to 140°C? Make any simplifying assumptions you think are justified, but state them. Figure P17.79
(a) Equation (17.12) gives the stress required to keep the length of a rod constant as its temperature changes. Show that if the length is permitted to change by an amount Δ L when its temperature changes by Δ T , the stress is equal to F A = Y ( Δ L L 0 − α Δ T ) where F is the tension on the rod, L 0 is the original length of the rod, A its cross-sectional area, α its coefficient of linear expansion, and Y its Young’s modulus. (b) A heavy brass bar has projections at its ends ( Fig. P17.79 ). Two fine steel wires, fastened between the projections, are just taut (zero tension) when the whole system is at 20°C. What is the tensile stress in the steel wires when the temperature of the system is raised to 140°C? Make any simplifying assumptions you think are justified, but state them. Figure P17.79
(a) Equation (17.12) gives the stress required to keep the length of a rod constant as its temperature changes. Show that if the length is permitted to change by an amount ΔL when its temperature changes by ΔT, the stress is equal to
F
A
=
Y
(
Δ
L
L
0
−
α
Δ
T
)
where F is the tension on the rod, L0 is the original length of the rod, A its cross-sectional area, α its coefficient of linear expansion, and Y its Young’s modulus. (b) A heavy brass bar has projections at its ends (Fig. P17.79). Two fine steel wires, fastened between the projections, are just taut (zero tension) when the whole system is at 20°C. What is the tensile stress in the steel wires when the temperature of the system is raised to 140°C? Make any simplifying assumptions you think are justified, but state them.
Consider a wire with a cross-section A and a length L.
The Young's modulus is given by:
Y =
LOF
A ƏL
T
Where F = F(T, L) is the tension in the wire.
The linear expansion coefficient is given by:
απ
1/ǝL
LOT
F
Give in expression for the change in tension in the wire with temperature in terms of the Young's modulus and the linear
expansion coefficient if the wire is kept at a fixed length.
A diver is at 5 meter depth in a fresh water lake. At that depth, the temperature is 15◦C. The pressure in the water at a depth d is given by p(d) = psurface + ρgd, where ρ is the liquid density, and g = 9.81m s−2is the gravitational constant.(a) The diver releases an air bubble of 1cm diameter. What is the diameter of the bubble when it reaches the surface where the temperature is 20◦C?Assume that the bubble temperature is always the same as the surroundingwater.(b) The diver stayed 1h at a 5m depth. The pressure in the diving tank went down from 250 bars to 50 bars. We assume that the volume of the lungs is 5L. Assuming that the water temperature is also 15◦C, how long could the diver have stayed underwater at 20m depth using the same amount of air?(c) The diver is at 5m depth and decides to surface. The air in the lungs is at a constant temperature of 37◦C. What fraction of the air in her/his lungs should the diver inhale/release to maintain a constant lung volume?
The density is obtained by dividing the mass by the volume. Since volume depends on temperature, so must density. Show that the change in density ∆ρ with the change in temperature ∆Tof temperature ∆T is given by∆ρ = -βρ∆T ,where β is the coefficient of volumetric expansion. Explain the meaning of the minus sign
Chapter 17 Solutions
University Physics with Modern Physics, Volume 1 (Chs. 1-20) and Mastering Physics with Pearson eText & ValuePack Access Card (14th Edition)
Physics for Scientists and Engineers: A Strategic Approach with Modern Physics (4th Edition)
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